“…6,7 In tokamak plasmas, long-tail electron distributions have been observed over the whole plasma column (edge, confinement region, and core) and related to different mechanisms and instabilities, such as magnetic reconnection, high-energy ions, non-local electron transport, neutral ionization, internal kink modes, sawtooth instabilities, electron fishbones, and plasma heating. [8][9][10][11] In particular, bi-Maxwellian distribution functions, an empirical model for long tail distributions used in the same context of the j-distributions in space plasmas, were fitted to the experimental data in the plasma edge during Ion Cyclotron Resonance Heating (ICRH) and Neutral Beam Injection (NBI) experiments. 12,13 In order to introduce non-thermal effects in the Boltzmann-based models, alternative fluid equations approximating different long-tail distribution functions by a series of Maxwellians, with the coefficients of proportionality determined by numerically fitting the experimental data, have been lately considered, especially in numerical simulations.…”